{"title":"库埃特流的边界驱动不稳定性","authors":"Dongfen Bian, Emmanuel Grenier, Nader Masmoudi, Weiren Zhao","doi":"10.1007/s00220-025-05401-7","DOIUrl":null,"url":null,"abstract":"<div><p>In this article, we prove that the threshold of instability of the classical Couette flow in <span>\\(H^s\\)</span> for large <i>s</i> is <span>\\(\\nu ^{1/2}\\)</span>. The instability is completely driven by the boundary. The dynamic of the flow creates a Prandtl type boundary layer of width <span>\\(\\nu ^{1/2}\\)</span> which is itself linearly unstable. This leads to a secondary instability which in turn creates a sub-layer.</p></div>","PeriodicalId":522,"journal":{"name":"Communications in Mathematical Physics","volume":"406 9","pages":""},"PeriodicalIF":2.6000,"publicationDate":"2025-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Boundary Driven Instabilities of Couette Flows\",\"authors\":\"Dongfen Bian, Emmanuel Grenier, Nader Masmoudi, Weiren Zhao\",\"doi\":\"10.1007/s00220-025-05401-7\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>In this article, we prove that the threshold of instability of the classical Couette flow in <span>\\\\(H^s\\\\)</span> for large <i>s</i> is <span>\\\\(\\\\nu ^{1/2}\\\\)</span>. The instability is completely driven by the boundary. The dynamic of the flow creates a Prandtl type boundary layer of width <span>\\\\(\\\\nu ^{1/2}\\\\)</span> which is itself linearly unstable. This leads to a secondary instability which in turn creates a sub-layer.</p></div>\",\"PeriodicalId\":522,\"journal\":{\"name\":\"Communications in Mathematical Physics\",\"volume\":\"406 9\",\"pages\":\"\"},\"PeriodicalIF\":2.6000,\"publicationDate\":\"2025-08-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Communications in Mathematical Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://link.springer.com/article/10.1007/s00220-025-05401-7\",\"RegionNum\":1,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"PHYSICS, MATHEMATICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Communications in Mathematical Physics","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1007/s00220-025-05401-7","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, MATHEMATICAL","Score":null,"Total":0}
In this article, we prove that the threshold of instability of the classical Couette flow in \(H^s\) for large s is \(\nu ^{1/2}\). The instability is completely driven by the boundary. The dynamic of the flow creates a Prandtl type boundary layer of width \(\nu ^{1/2}\) which is itself linearly unstable. This leads to a secondary instability which in turn creates a sub-layer.
期刊介绍:
The mission of Communications in Mathematical Physics is to offer a high forum for works which are motivated by the vision and the challenges of modern physics and which at the same time meet the highest mathematical standards.